Step 1: Understanding the problem.
Since the bomb is initially at rest, the total momentum of the system is zero. After the explosion, the vector sum of the momenta of the three parts must still be zero.
\[
\vec{P_1} + \vec{P_2} + \vec{P_3} = 0
\]
Step 2: Apply the given momentum values.
The momentum of the first two parts is given as \( \vec{P_1} = -3P_i \) and \( \vec{P_2} = 2P_j \). Let the momentum of the third part be \( \vec{P_3} = P_3 \).
Step 3: Apply the Pythagorean theorem.
Since the total momentum is zero, we can use the Pythagorean theorem to find the magnitude of the third momentum \( P_3 \). We have:
\[
P_3 = \sqrt{P_1^2 + P_2^2}
\]
Substituting the given values:
\[
P_3 = \sqrt{(-3P)^2 + (2P)^2} = \sqrt{9P^2 + 4P^2} = \sqrt{13P^2} = \sqrt{13} P
\]
Step 4: Conclusion.
Thus, the magnitude of the momentum of the third part is \( \sqrt{13} P \), which corresponds to option (B).